Microwaves Turn a Superconductor into a Magnet ✛ ✎

Original: "Microwave-Induced Optomagnetism in High-Temperature Superconductors"
arXiv:2608.31127v1 · 2026-08-31 · arXiv non-exclusive · independent analysis · 2 min
For the first time, a static magnetic field has been created in a superconductor using microwave radiation.

A microwave oven heats food, but in the lab, microwaves have done something different: they turned a superconductor into a permanent magnet. A 300-nanometer-thick film of yttrium barium copper oxide, cooled to 80 kelvin, responded to 5-gigahertz radiation. This is the first observation of the stationary inverse Faraday effect in a high-temperature superconductor.

The essence of the effect is simple: light with circular polarization, meaning an electric field that rotates, makes electrons move in circles. In a normal conductor, these circular currents quickly die out, but in a superconductor they encounter no resistance. A permanent magnetic field arises, as if an invisible electromagnet had appeared inside the material. The key difference from ordinary coils is the absence of wires and heat losses.

The key trick of the experiment is polarization modulation. The radiation was switched between left and right circular polarization 83,000 times per second, and the Hall voltage changed synchronously. Linearly polarized control gave no signal, ruling out heating.

As power increased, the signal grew until the calculated internal field exceeded 0.82 micronewtons per meter, the lower critical field at which vortices of magnetic flux begin to penetrate the superconductor. At that point, the signal dropped sharply to zero, and at even higher power, narrow peaks appeared at the third and fourth harmonics of the vortex lattice frequency. The material seemed to reconfigure, transitioning from a homogeneous state to an ordered vortex structure.

The conversion efficiency reached 1.75 tesla per watt per square centimeter. This is several orders of magnitude higher than optical analogs. For comparison, a neodymium magnet produces about 1.2 tesla at its surface.

The practical value is obvious. In superconducting quantum circuits, magnetic biasing is currently done with inductive lines, which heat up and cause crosstalk. Microwave control of magnetization could replace these lines and reduce qubit decoherence. Moreover, the method is suitable for spectroscopy of vortex dynamics in type-II superconductors.

The microwave oven in the kitchen heats soup, but in a physics lab, it spins an electronic "gyroscope" without friction. The superconductor, like a frictionless top, keeps spinning after the external torque is removed, but now in the form of a permanent magnetic field. Perhaps soon such fields will control quantum computers contactlessly and without losses.

The effective optomagnetic conversion of 1.75 T/(W/cm²) means that microwave radiation with a power of just 1 W per square centimeter creates a magnetic field of nearly two tesla. For comparison, a typical neodymium magnet provides about 1.2 T at its surface.

\langle \tilde{M} \rangle = \gamma(\omega) \operatorname{Im}[\tilde{E} \times \tilde{E}^*]
Magnetization is proportional to the gyration coefficient and the imaginary part of the cross product of the electric field with its complex conjugate
\gamma(\omega) = \frac{n_s e^3}{4 m_s^{*2} \omega^3} + \frac{n_n e^3}{4 m_n^{*2} \omega^3} \frac{\omega^2 \tau_n^2}{1 + \omega^2 \tau_n^2}
Contribution from the superconducting condensate and normal quasiparticles; at microwave frequencies, the normal component contribution is suppressed by a factor of 10^7
\tilde{\rho}_H = \frac{\tilde{\sigma}_{xy}}{\tilde{\sigma}_{xx}^2 + \tilde{\sigma}_{xy}^2}
Hall resistance is expressed through the gyromagnetic conductivities of both fluids
Scientists
Michael FaradayHendrik LorentzSatyendra Nath BoseJohn BardeenFelix BlochGeorg Ohm
Concepts
magnetophotonic effects Faraday's law of electromagnetic induction Faraday effect light induced superconductivity magneto optical kerr effect cryogenic microwave measurement microwave signal magnetic vortex thin film superconductivity superconducting phase transition flux pinning magnetic refrigeration high temperature superconductor thermoelectric device superconducting wire optical vortex ferroelectric antiferromagnetic order Wave Function Collapse faraday constant